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Related Concept Videos

MOSFET: Enhancement Mode01:22

MOSFET: Enhancement Mode

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Enhancement-mode MOSFETs are pivotal components in electronics, distinguished by their capacity to act as highly efficient switches. They are part of the larger family of metal-oxide Semiconductor Field-Effect Transistors (MOSFETs). They are available in two types: p-channel and n-channel, each tailored to specific polarity operations.
In their basic form, enhancement-mode MOSFETs are typically non-conductive when the gate-source voltage (Vgs) is zero. This default 'off' state means no...
448
Biasing of Metal-Semiconductor Junctions01:27

Biasing of Metal-Semiconductor Junctions

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Biasing metal-semiconductor junctions involves applying a voltage across the junction. Specifically, the metal is connected to a voltage source, while the semiconductor is grounded. This technique is essential for controlling the direction and magnitude of current flow in electronic devices, including diodes, transistors, and photovoltaic cells.
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
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Biasing of FET01:22

Biasing of FET

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Biasing a Junction Field Effect Transistor (JFET) is crucial for setting operational parameters and ensuring efficient functioning in electronic circuits. JFETs are characterized by using a single carrier type in N-channel or P-channel configurations, where the channel is surrounded by PN junctions. These junctions are central to the device's ability to control current flow.
In an N-channel JFET, the structure consists of N-type material forming the channel on a P-type substrate, with the...
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MOSFET: Depletion Mode01:20

MOSFET: Depletion Mode

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Depletion-mode MOSFETs represent a unique subset of MOSFET technology, functioning fundamentally differently from their enhancement-mode counterparts. Unlike enhancement MOSFETs, which require a positive gate-source voltage (Vgs) to turn on, depletion-mode MOSFETs are inherently conductive and "normally on" devices.
The primary characteristic of depletion-mode MOSFETs is their ability to conduct current between the drain and source terminals without gate bias. This inherent conductivity...
450
Biasing of P-N Junction01:16

Biasing of P-N Junction

737
The operation of a p-n junction diode involves various biasing conditions, including forward bias, reverse bias, and equilibrium.
In equilibrium, no external voltage is applied across the p-n junction. The depletion region is formed at the junction interface due to the diffusion of carriers, which leaves behind charged dopants, acceptors on the p-side, and donors on the n-side. These immobile charges create an electric field that prevents further diffusion of carriers. The related energy band...
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Metal-Semiconductor Junctions01:24

Metal-Semiconductor Junctions

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The contact of metal and semiconductor can lead to the formation of a junction with either Schottky or Ohmic behavior.
Schottky Barriers
Schottky barriers arise when a metal with a work function (Φm) contacts a semiconductor with a different work function (Φs). Initially, electrons transfer until the Fermi levels of the metal and semiconductor align at equilibrium. For instance, if Φm > Φs, the semiconductor Fermi level is higher than the metal's before contact. The...
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Updated: Aug 23, 2025

Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform
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Steep-slope transistors enabled with 2D quantum coupling stacks.

Parameswari Raju1,2, Hao Zhu3, Yafen Yang3

  • 1Department of Electrical and Computer Engineering, Fairfax, George Mason University, Fairfax, VA 22030, United States of America.

Nanotechnology
|November 1, 2022
PubMed
Summary
This summary is machine-generated.

Researchers developed steep-slope transistors using 2D materials like graphene in the gate stack. This innovation, validated by simulations and experiments, promises enhanced performance for future scaled transistors.

Keywords:
TMDCdensity functional theoryquantum capacitancequantum couplingsteep-slope transistors

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Area of Science:

  • Materials Science
  • Semiconductor Physics
  • Nanotechnology

Background:

  • Transistor scaling faces limitations due to the Boltzmann limit for subthreshold slope (SS).
  • Steep-slope transistors with SS below the Boltzmann limit are crucial for continued device scaling and improved energy efficiency.

Purpose of the Study:

  • To investigate the use of 2D quantum materials in gate stacks for fabricating steep-slope transistors.
  • To theoretically and experimentally validate the effectiveness of incorporating materials like graphene into MoS2 transistors.

Main Methods:

  • Fabrication of MoS2 transistors with an inserted graphene layer in the gate stack.
  • Application of density functional theory (DFT) to simulate SS in devices with various 2D materials (graphene, germanene, 2D topological insulators).
  • Experimental characterization of fabricated graphene/MoS2 transistors.

Main Results:

  • Experimental fabrication of steep-slope MoS2 transistors with a subthreshold slope of 49.2 mV/decade.
  • DFT simulations predicted a steep SS of 27.2 mV/decade for graphene/MoS2 devices.
  • Simulations indicated an exceptionally steep SS of 8.6 mV/decade for WTe2/MoS2 devices.

Conclusions:

  • Incorporating 2D quantum materials into gate-channel stacks is an effective strategy for achieving steep-slope transistors.
  • The combination of specific 2D materials can significantly reduce the subthreshold slope, enabling further transistor scaling.
  • This approach offers a pathway to extend transistor scaling while maintaining exceptional device performance.